canonical setting

Weakly smooth log-concave

VV convex, V(x)V(y)βsxys\lVert\nabla V(x)-\nabla V(y)\rVert\le\beta_s\lVert x-y\rVert^s, s[0,1]s\in[0,1].

Upper and lower bounds

Comparison table

4 scoped results. Tildes suppress logarithmic factors.

Edit table
Best-known and comparison results for Weakly smooth log-concave
ResultAlgorithm or modelComplexityGuaranteeOracle / startAssumptions and notesReviewSources
best upperFORS + proximal samplerO~(βs2/(1+s)ds/(1+s)R02/ε2)\widetilde O(\beta_s^{2/(1+s)}d^{s/(1+s)}R_0^2/\varepsilon^2)KLε2\operatorname{KL}\le\varepsilon^2First-order + proximal implementationW2(μ0,π)=R0W_2(\mu_0,\pi)=R_0Hölder gradient and the implementation assumptions in the theorem.Provisional transcription. At s=0s=0 it gives the displayed nonsmooth endpoint.Citedpreprint
lower unknownMatching Hölder-model lower boundUnknownSame KL and first-order modelHölder first-order oracleW2(μ0,π)=R0W_2(\mu_0,\pi)=R_0No matching result located in the reference corpus.Open literature-check item.Unverifiedno primary source
upperAveraged LMCO(L2R02/ε4)O(L^2R_0^2/\varepsilon^4)KLε\sqrt{\operatorname{KL}}\le\varepsilonSubgradient / LMC stepW2(μ0,π)=R0W_2(\mu_0,\pi)=R_0VV convex and LL-Lipschitz.Checked nonsmooth Euclidean baseline.Checkedmonograph
upperNonsmooth mirror-LangevinO(L2Dϕ(π,μ0+)/ε4)O(L^2D_\phi(\pi,\mu_{0+})/\varepsilon^4)KLε\sqrt{\operatorname{KL}}\le\varepsilonDual-norm subgradient + mirror mapBregman-divergence scaleϕ\phi one-strongly convex in the primal norm.Not directly comparable to the Euclidean R0R_0 rows.Checkedmonograph

Scope

The Hölder exponent interpolates between the smooth case s=1s=1 and the Lipschitz/nonsmooth endpoint s=0s=0 (up to the usual subgradient interpretation). Mirror rows use their own norm and Bregman geometry and are shown as separate comparators.

Lower bounds

No matching lower bound for the full Hölder-gradient model is recorded in the current reference corpus.